JP3465946B2 - Load cell temperature compensation method and apparatus - Google Patents

Description

Detailed Description of the Invention

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a load cell temperature compensation method and apparatus for compensating an output change due to temperature of a strain gauge type load cell used as a weight sensor of a weighing device.

[0002]

2. Description of the Related Art In order to compensate the temperature characteristic of the zero point (zero temperature compensation) in the unloaded state in which no load is applied to the conventional strain gauge type load cell, for example, a strain gauge G ₄ of a bridge circuit shown in FIG. 11 is used. It is necessary to insert a copper wire resistor r ₁ whose resistance value changes in accordance with a change in temperature in series with.

However, the temperature coefficients (non-loaded state) of the strain gauges G _{1 to} G ₄ attached to the load cells are slightly different for each load cell, and this difference in temperature coefficient is the zero point of each load cell. Is the main cause of the difference in the temperature characteristics. Therefore, it is necessary to adjust the resistance value (length) of the copper wire resistance r ₁ to be inserted into the bridge circuit for each load cell and solder it. However, adjusting and cutting the copper wire resistance r ₁ to a desired resistance value must be done manually, and there is a problem that it takes a lot of time and labor.

Therefore, an invention that solves this problem is disclosed in
In the microcomputer 9 shown in FIG. 12, V≈V ₀ (1-α ₁ t) ... (1) ΔV = ΔV ₀ (1 + β ₁ t). .. (2) is stored in advance. When compensating for the zero point, the following steps are executed to compensate the zero point. However, V is the input voltage of the bridge circuit 1 at the temperature t (input terminals 1a, 1
b)), V ₀ is the input voltage of the bridge circuit 1 at 0 ° C., α ₁ is the temperature coefficient of the temperature sensitive resistor 2, t is the temperature of the load cell 3, and ΔV is the bridge circuit 1 at the temperature t.
Is the zero point change amount, ΔV ₀ is the zero point change amount of the bridge circuit 1 at 0 ° C., and β ₁ is the temperature coefficient of the bridge circuit 1.

(A) First, at the timing of compensating for the zero point, the microcomputer 9 sends a switching signal S to the switch means 5. As a result, the switch means 5 of FIG. 12 is closed, the multiplexer 7 is connected to the amplifier circuit 4'side, the input voltage V of the bridge circuit 1 is input to the amplifier circuit 4 ', and the output of the amplifier circuit 4'is , Multiplexer 7, and A / D converter 8 to be input to the microcomputer 9.

(B) Next, the computer 9 substitutes the input voltage V into the equation (1) to calculate the load cell temperature t, substitutes the calculated temperature t into the equation (2), and at the temperature t. A zero change amount ΔV at the temperature t of the bridge circuit 1 is obtained.

(C) Next, the computer 9 converts the variation ΔV into a digital value at a predetermined conversion rate,
The value is subtracted from the zero point of the scale stored in the computer 9 to correct the zero point change due to the temperature of the load cell.
As a result, the zero point of the balance is set to a value that does not depend on the temperature.

FIG. 13 shows another embodiment of the present invention. Reference numeral 10 shown in the figure is a voltage dividing circuit, which is formed of a precision resistor having good temperature characteristics, and is designed to output a predetermined constant voltage that is not affected by temperature. Then, the input voltage V of the voltage dividing circuit 10 is input to the amplifier circuit 4 via the switch means 5, and the computer 9 calculates the temperature t in the same manner as above. Then, based on this temperature t, the variation Δ
V is calculated to correct the zero point change due to the temperature of the load cell.

[0009]

In the zero correction device shown in FIG. 12, the input voltage V to the amplifier circuit 4'is the excitation voltage V.
It is a voltage obtained by subtracting the voltage drop due to the temperature sensitive resistor 2 from _ex, which is a voltage slightly lower than the excitation voltage V _ex . That is, for example, the resistance value R _s of the temperature sensitive resistor 2 is about 48.
Each resistance value (G _{1 to} G ₄ ) of Ω and strain gauge 3 is about 35.
Assuming that 0Ω and the excitation voltage V _ex are 10 V, the input voltage V is
It becomes about 8.8V.

The reason why the resistance value R _s of the temperature sensitive resistor 2 for compensating for the span change is set to about 48Ω is that the resistance value (G _{1 to} G ₄ ) of the strain gauge 3 is 350Ω, and the span compensation is Rate of change in span of load cell without condition α ₂ = 60
0 ppm / ° C, temperature coefficient of resistance of temperature sensitive resistor 2 β ₂ = 500
Since it can be calculated that the resistance value of the temperature sensitive resistor 2 is R _s = α ₂ G ₁ / (β ₂ −α ₂ ) = 600 × 350 / (5000−600) ≈48 (Ω), when it is 0 ppm / ° C. Is.

By the way, it is necessary to make the power supply voltage V _ey of the analog signal processing circuits such as the amplifier circuit 4 ', the filter circuit 6 and the A / D converter 8 and the excitation voltage V _ex of the bridge circuit 1 common. Necessary to reduce the cost of the circuit.

However, when the power supply voltage V _ey of the analog signal processing circuit is set to 10V, the amplification factor k _x of the amplification circuit 4'is 10/8 because the input voltage V input to the amplification circuit 4'is 8.8V. It is necessary to be less than 0.8 ≈ 1.1, and the amplification factor k
There is a problem that _x cannot be designed to a large value. That is, if the amplification factor k _x cannot be set to a large value, the amount of change in the output voltage of the amplifier circuit 4 ′ based on the change in temperature t will be small, and the temperature t must be measured based on this small amount of change. Therefore, there is a problem that the temperature t cannot be accurately measured, and as a result, the zero point correction cannot be accurately performed. Therefore, in order to perform the zero point correction accurately, it is necessary to separately provide the power source voltage V _ey larger than the power source voltage (excitation voltage V _ex ) of the bridge circuit 1 for the amplifier circuit 4 ′ and the like. The problem is that it becomes complicated and expensive.

However, in the other embodiment of the present invention shown in FIG. 13, since the voltage dividing circuit 10 is provided, the bridge circuit 1
The power supply voltage (excitation voltage V _ex ) of the amplifier circuit and the power supply voltage V _ey of the amplifier circuits 4 and _4'can be made common, but the voltage dividing circuit 10 includes a precision resistor whose resistance value does not change with temperature. There is a problem that it is expensive because it is necessary.

An object of the present invention is to provide a temperature compensating method for a load cell and a device therefor, which can accurately perform zero point correction with respect to a temperature change by using an inexpensive device.

[0015]

According to a first aspect of the present invention, there is provided a temperature compensating method for a load cell, wherein a strain sensing type load cell having a strain gauge in a bridge circuit is provided with a temperature sensitive element on a strain generating element.
One end of the temperature sensitive element is connected to one input end of the bridge circuit, a power source is connected between the other end of the temperature sensitive element and the other input end of the bridge circuit, and the output end of the bridge circuit is connected. In the temperature compensating method for the load cell, the voltage difference of 1 is amplified by the first amplifier, the voltage of one output end is amplified by the second amplifier, and the voltage is supplied to the first and second amplifiers from the power source. , The zero point change amount C _M generated at both output ends of the bridge circuit based on the temperature change, C _M = C
_{1 - [(A 2 -A 1} ) / (B 2 -B 1)] _{[D-D 1} -
_{(D 2 -D 1) (C} -C 1) / (C 2 -C 1) ] (where, _{C 1} is the output voltage of the first amplifier when the article on the load cell at a reference temperature is not loading A certain load voltage, C ₂ is the load voltage when a weight of weight m is loaded on the load cell at the reference temperature, C is the load voltage when a certain load is loaded on the load cell at an arbitrary temperature, D1 Is a temperature voltage which is an output voltage of the second amplifier when an article is not loaded on the load cell at the reference temperature, D2 is the temperature voltage when a weight of weight m is loaded on the load cell at the reference temperature, D is the temperature voltage when a certain load is loaded on the load cell at the arbitrary temperature, and A ₁ is an article is not loaded on the load cell at the first temperature. Load voltage, A ₂ is the load voltage when an article is not loaded on the load cell at a second temperature, and B ₁ is the temperature voltage when an article is not loaded on the load cell at a first temperature , B ₂ is second
The temperature voltage when the load cell is not loaded with an article) and the zero point correction of the load voltage generated at both output ends of the bridge circuit based on the zero point change amount. And stages.

A second aspect of the present invention is the load cell temperature compensation method according to the first aspect, wherein the temperature sensitive element electrically corrects an output span due to the temperature of the load cell.

According to a third aspect of the present invention, there is provided a temperature compensating device for a load cell, wherein a bridge circuit including a strain gauge provided on a strain-generating body of the load cell and the strain-generating body, one end of which is one input end of the bridge circuit. A temperature-sensitive element connected to
A voltage difference is supplied between the power supply connected between the other end of the temperature sensing element and the other input end of the bridge circuit and the output end of the bridge circuit, and a voltage is supplied from the power supply. A second amplifier for amplifying a voltage at one output end of the bridge circuit and a voltage supplied from the power supply.
And the zero point change amount C _M generated at both output terminals of the bridge circuit based on the temperature change as C _M = C <sub>1
- [(A 2 -A 1)</sub> / (B 2 -B 1)] _{[D-D 1} -
_{(D 2 -D 1) (C} -C 1) / (C 2 -C 1) ] (where, _{C 1} is the output voltage of the first amplifier when the article on the load cell at a reference temperature is not loading A certain load voltage, C ₂ is the load voltage when a weight of weight m is loaded on the load cell at the reference temperature, C is the load voltage when a certain load is loaded on the load cell at an arbitrary temperature, D1 Is a temperature voltage which is an output voltage of the second amplifier when an article is not loaded on the load cell at the reference temperature, D2 is the temperature voltage when a weight of weight m is loaded on the load cell at the reference temperature, D is the temperature voltage when a certain load is loaded on the load cell at the arbitrary temperature, and A ₁ is an article is not loaded on the load cell at the first temperature. Load voltage, A ₂ is the load voltage when an article is not loaded on the load cell at a second temperature, and B ₁ is the temperature voltage when an article is not loaded on the load cell at a first temperature , B ₂ is second
At zero temperature change amount calculation means for calculating the temperature voltage when the load cell is not loaded with the article), and the load voltage generated at both output ends of the bridge circuit based on the zero point change amount. And a correction means for correcting the zero point.

According to a fourth aspect of the present invention, in the temperature compensating device for a load cell according to the third aspect, the temperature sensing element is set to a resistance value that electrically corrects an output span due to the temperature of the load cell. .

[0019]

According to the first and third aspects of the invention, the temperature voltage is generated at one output end of the bridge circuit, and the load voltage is generated at both output ends of the bridge voltage. Then, the temperature voltage and the load voltage are arithmetically processed to calculate the zero point change amount generated at both output ends of the bridge circuit based on the temperature change. Then, the zero point correction is performed by subtracting or adding the zero point change amount from the weight voltage.

Since the temperature voltage (eg, e ₂ ) generated at one output end of the bridge circuit is less than 1/2 of the power supply voltage (eg, E ₁ ) of the bridge circuit,
A power supply voltage E ₁ of the bridge circuit, even when sharing the power supply voltage E ₁ such as an amplifier for amplifying the temperature voltage e _2,
The amplification factor k ₂ of the amplifier can be designed to E ₁ / e ₂ > 2.

According to the second and fourth inventions, the temperature-sensitive element of the first and third inventions electrically corrects the output span change due to the temperature of the load cell.

[0022]

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS A first embodiment of the present invention will be described with reference to the drawings. FIG. 1 is a block diagram showing an electric circuit of a weighing device equipped with a temperature compensating device for a load cell of this embodiment. As shown in the figure, a temperature sensitive element 12 is connected in series to the input side of the bridge circuit 11 of the load cell, and a change in the resistance value R _S of the temperature sensitive element 12 causes an output span change of the bridge circuit 11 with respect to a temperature change of the load cell. This is a compensation structure.

The bridge circuit 11 is composed of, for example, four strain gauges G (G _{1 to} G ₄ ) provided in a conventionally known strain generating body, and the temperature sensing element 12 is a temperature coefficient of the strain gauge G. copper sufficiently large temperature coefficient than nickel is formed of titanium or the like, the resistance value R _S, the bridge circuit 11
It is set to a value that can cancel out the output span change due to the temperature. For example, if the resistance value R of the strain gauge G is 350Ω, the resistance value R _S of the temperature sensing element 12 is necessarily about 48 in order to cancel the output span change as described in the conventional example.
It becomes Ω.

Further, both output terminals 1 of the bridge circuit 11
The weighted voltages e ₁ and e ₂ generated at 4 and 15 are generated by the amplifier 16
To the filter circuit 17, and the noise component is removed. The output of the filter circuit 17 is A / A via the switch SW1 of the switch circuit 18.
The digital output is input to the D conversion circuit 19, and the digital output is input to a central processing unit (hereinafter, referred to as CPU 20) to be subjected to predetermined arithmetic processing.

Then, the temperature voltage e ₂ generated at one output end 15 of the bridge circuit 11 is input to the CPU 20 via the amplifier 21 and the switch SW2 and subjected to predetermined arithmetic processing. In addition, the switch SW1 of the switch circuit 18,
SW2 is configured to be controlled to be switched between an a-contact side and a b-contact side by a switching signal S output from the CPU 20. That is, in the weight measurement mode for weighing, SW1 is ON and SW2 is OFF, and in the temperature measurement mode for measuring temperature, SW1 is OFF, SW2.
Turns on.

When compensating for the zero change of the load cell, the temperature sensitive element 12 is used as a temperature sensor for detecting the temperature of the load cell, and the resistance value R _{S of} this temperature sensor is used.
The temperature voltage e ₂ generated at the output end 15 that changes based on the change of the
20 to be processed. Therefore, another temperature sensitive element for compensating the zero change of the load cell is not required. In addition,
The amplifiers 16 and 21 are differential amplifiers.

However, the power supply voltage of the bridge circuit 11 shown in FIG. 1, the amplifiers 16 and 21, the filter circuit 17, and the A / D
The power supply voltages of the analog circuits such as the conversion circuit 19 are, for example, E ₁ (= 10 V), and are taken out from the same power supply circuit. However, this common power supply voltage E ₁ is
A voltage other than 10V may be used.

Next, the temperature compensation of the output span by the temperature compensating device having the above-mentioned structure will be described. When the metering device shown in FIG. 1 is powered on, an exciting voltage E _{1 that} is independent of temperature is applied to the bridge circuit 11 and the temperature sensing element 12,
As a result, the bridge circuit 11 outputs a weighted voltage (e ₁ -e ₂ ) proportional to the strain amount of the flexure element. When the load cell temperature gradually rises for some reason, the Young's modulus of the flexure element decreases and the strain amount of the flexure element increases. As a result, the load voltage A in the loaded state of the bridge circuit 11 is As shown in 4, the temperature rises as the temperature t of the load cell rises. That is, the output span of the load cell increases in relation to the load and the load cell output (e ₁ -e ₂ ). Further, the resistance value R _{S of the} temperature sensitive element 12 also rises as the temperature rises. Then, the excitation voltage E _c (see FIG. 3) applied to the bridge circuit 11 decreases due to the increase in the resistance value of the temperature sensitive element 12, so that the load voltage A (= e ₁ −e ₂ ) of the bridge circuit 11 is reduced. Goes down.

However, the resistance value R _s of the temperature sensitive element 12 is designed so that the rate of increase of the load voltage A and the rate of decrease of the load voltage A due to the increase of the resistance value of the temperature sensitive element 12 are substantially equal. Therefore, the weighted voltage A of the bridge circuit 11 is generated as an output that is not affected by temperature by canceling these span changes. Further, when the temperature of the load cell decreases, the change of the load voltage A due to the temperature is similarly canceled by the action opposite to the above. Therefore, the output span of the load cell is output as being electrically completely temperature compensated at the load voltage A of the bridge circuit 11.

Next, the temperature compensation of the zero point by the temperature compensating device having the above construction will be described. In the weighing device shown in FIG. 1, in the state of the weight measurement mode, the switch SW1 shown in FIG.
2 is set to the OFF state, and the bridge circuit 11
Of the load voltage A (= e ₁ − generated at the output terminals 14 and 15 of the
e ₂ ) is an amplifier 16, a filter circuit 17, a switch S
The signal is input to the CPU 20 via the W1 and A / D conversion circuit 19, and the input signal is arithmetically processed by the CPU 20 to calculate the weight. For example, in an electronic scale, the bridge circuit 11 input in the initial state immediately after the power is turned on.
The load voltage A is stored as the zero point of the scale, and in the combination scale, the load voltage A at the time of no load input at the time of zero adjustment is stored as the zero point of the scale.

However, since the zero point of the scale fluctuates depending on the temperature, the CPU 20 regularly or irregularly executes temperature compensation of the zero point based on the principle described below.

Now, in the temperature compensation stage of the zero point at the time of manufacturing the load cell, as shown in FIGS. 4 and 5, the load voltage A (= e ₁ -e ₂ ) in the unloaded state at the temperature t = t _1.
= A ₁ , temperature voltage B (= e ₂ ) = B ₁ , and temperature t
= Load voltage A (= e ₁ −e ₂ ) = t ₂ at no load =
A ₂ and temperature voltage B (= e ₂ ) = B ₂ are obtained. The measured voltages A ₁ , A ₂ , B ₁ , and B ₂ are stored in the RAM or EEPROM of the storage unit 22 shown in FIG.

Therefore, the zero point (load voltage A) of the load cell when there is no load is (A ₂ −A ₁ ) / (t ₂ per 1 ° C. temperature.
-T ₁ ) Change in bolt. The temperature voltage B changes by (B ₂ −B ₁ ) / (t ₂ −t ₁ ) volt per 1 ° C. of temperature. That is, when the strain gauges G (G _{1 to} G ₄ ) are not strained (no-load state), that is, when the resistance values of the strain gauges G _{1 to} G ₄ are R (constant), the temperature voltage B The change amount ΔA of the load voltage A can be calculated on the basis of the change amount ΔB of the load voltage A, and thus the zero point correction of the load voltage A can be performed.

However, when a load is applied to the load cell, strain is generated in the strain gauges G _{1 to} G ₄ , and as shown in FIG. 3, each resistance value is (R-ΔR) or (according to the compressive force and the tensile force). R + ΔR), the temperature voltage e ₂ at the output end 15 of the bridge circuit 11 becomes e ₂ = (R + ΔR) · E _c / 2R ··· (3), and the temperature voltage e ₂ is equal to the temperature t. It will change under the influence of load other than the influence. However, E _c is an excitation voltage generated at the input terminals 24 and 25 of the bridge circuit 11.

Therefore, a method for detecting the temperature voltage e ₂ with the influence of the load removed even when an arbitrary load is applied to the load cell will be described below. First, the load voltages C ₁ and C ₂ shown in FIG. 6 and the temperature voltages D ₁ and D ₂ shown in FIG. 7 are obtained at the stage of span adjustment during balance adjustment. The temperature at this time is the reference temperature t _x . That is, first, for example, the load voltage C when the article is not placed on the platform on which the article to be weighed is placed.
_{(= E 1 -e 2) =} C 1, temperature voltage _{D (= e 2) = D} 1
To measure. Next, the load voltage C = C ₂ and the temperature voltage D = D ₂ when a weight of weight m is mounted on the mounting table are measured. However, the weight M shown in FIGS. 6 and 7 is the tare load of the balance. Then, these measured voltages C ₁ , C ₂ , D ₁ , D
₂ is a RAM or EEP as the storage unit 22 shown in FIG.
Store in ROM. Further, the span coefficient k is calculated from m / (C ₂ −C ₁ ) = k, and the span coefficient k is also stored.

Next, assuming that the load voltage when a certain load is applied at an arbitrary temperature t is C and the temperature voltage is D, this temperature voltage D is the same as the temperature voltage at the reference temperature t _x . the difference becomes H, the variation H of the temperature voltage D is, H = D - in _{[(D 2 -D 1) (C} -C 1) / (C 2 -C 1) + D 1 ] ... (4) You can ask. That is, D of the first term of the equation (4)
Is the temperature voltage when the temperature is t, a load is applied to the load cell, and the load voltage is C, and the second term is
This is the temperature voltage when the temperature is t _x , a certain load is applied to the load cell, and the load voltage is C. Therefore, by taking this difference, the change amount H of the temperature voltage D in which the influence of the load voltage C is removed Can be calculated. In addition, in FIG.
It is a figure showing the relationship between H and temperature t, and H shown in this FIG.
The straight line is a straight line of the temperature voltage B shown in FIG. 5 translated downward by B _x .

By the way, this change amount H is obtained by moving the temperature voltage B at the output end 15 of the bridge circuit 11 in parallel downward by B _x , so that the temperature per 1 ° C. (B ₂ −
B ₁₎ the change of / (t ₂ -t _1). Therefore, H / [(B ₂ −B ₁ ) / (t ₂ −t ₁ )] = Δt (5), the amount of temperature change Δt of the temperature t with respect to the reference temperature t _x.
Can be calculated.

Further, from FIG. 4 showing the load voltage A, the fact that the zero point changes by (A ₂ −A ₁ ) / (t ₂ −t ₁ ) per 1 ° C. of temperature indicates that it is an adjusting step at the time of manufacturing the load cell. In the temperature measurement mode, _if the temperature variation Δt of the temperature t at that time with respect to the reference temperature t _x can be calculated from the equation (5), the zero point variation of the load voltage A based on this temperature variation Δt becomes , [(A ₂ −A ₁ ) / (t ₂ −t ₁ )] · Δt ··· (6). Therefore, using the tare load voltage C ₁ under the reference temperature t = t _x at the time of span adjustment at the time of balance adjustment, the tare load voltage C _M after the temperature change of Δt is newly generated as follows. By performing the calculation, it is possible to remove the influence of the temperature from the load voltage C of the load cell whose zero point has changed. That is, tare weight voltage C _M is, C _M = C ₁ - obtained as _{[(A 2 -A 1) / (} t 2 -t 1) ] · Δt ··· (7).

Then, the expressions (4) and (5) are substituted for the expression (7).
Enter, C_MIs   C_M= C₁-[(A₂-A₁) / (T₂-T₁)] ・ [(T₂-T₁) / (B ₂ -B₁)] ・ [DD₁-(D₂-D₁) (C-C₁) / (C₂-C₁)]       = C₁-[(A₂-A₁) / (B₂-B₁)] ・ [DD₁-(D₂-D ₁ ) (C-C₁) / (C₂-C₁)] (8) Can be obtained with. The second term on the right side of equation (8) is the temperature change.
The correction amount of the zero point of the load cell by the component Δt is shown.
Moreover, this temperature change Δt can be calculated by the equation (4).
The influence based on the weight voltage C is removed. this
A means for calculating the second term on the right side of the equation (8) (see FIG. 10).
Step 212) is the zero point change amount calculation according to claim 3.
It is a means. Therefore, it depends on the load cell from the formula (5).
The amount of temperature change Δt that removes the influence of the load is obtained, and this temperature
By substituting the amount of temperature change Δt into equation (7),
New zero point (tare load) that compensates for the zero point error caused by
Heavy voltage C_M) Can be calculated. Is this equation (7)
Means for calculating the equation (8) derived from
212) is the correction means according to the third aspect.

Thereafter, the weight W applied to the load cell is accurately calculated by using the zero point (tare load voltage) C _M obtained by the equation (8) and the span coefficient k obtained and stored when the load cell is manufactured. Can be measured. That is, the weight W can be obtained from W = k (C-C _M ) ... (9).

Next, referring to the flow chart of FIG. 9, the procedure of span adjustment at the time of balance adjustment, and as shown in FIG. 10, each value C ₁ obtained by this span adjustment,
A procedure for performing zero point correction in the weighing mode using C ₂ , D ₁ , D ₂ and the span coefficient k will be described.

First, the flowchart of FIG. 9 will be described.
A program for executing the contents of this flowchart is stored in, for example, an EPROM, and the CPU 20 operates according to this program. First, the operator turns on the power supply voltage of the weighing device shown in FIG. Then, the CPU 20 turns on the switch SW1 shown in FIG.
The switch SW2 is turned off (step 100), and the load voltage C ₁ generated at the output terminals 14 and 15 of the bridge circuit 11 is read in the unloaded state (the state in which the weight is not placed on the mounting table) (step 102). ). And CP
U20 turns off the switch SW1 and turns on the switch SW2 (step 104), and reads the temperature voltage D ₁ generated at the output end 15 of the bridge circuit 11 in the no-load state (state in which no weight is placed). (Step 1
06). Next, the operator places a weight of weight m on the mounting table (step 108), and then the CPU 20 turns on the switch SW1 and turns off the switch SW2 (step 110), and bridges under the load of weight m. Weighted voltage C ₂ generated at the output terminals 14 and 15 of the circuit 11
(Step 112), and then switch SW1
OFF and switch SW2 ON (step 11
4), the output terminal 1 of the bridge circuit 11 under the same load condition
The temperature voltage D ₂ generated in step 5 is read (step 11
6). Then, the CPU 20 calculates the span coefficient k from the weights m, C ₁ and C ₂ and reads this k (step 118), after which the switch SW1 is turned on and the switch SW2 is turned off to end the span adjustment. (Step 120). However, the temperature t at this time is constant.

Next, with reference to the flow chart of FIG. 10, a procedure for correcting the zero point when measuring the weight of an article will be described. First, the CPU 20 measures the temperature measurement time with the temperature measurement timer provided in the CPU 20, and determines whether or not the temperature measurement timing has come (step 200). Then, the temperature measurement time comes, and if YES is determined, the temperature measurement mode is set, and the switch SW1 is turned off.
F, switch SW2 is turned on (step 202),
Temperature voltage D _P generated at the output end 15 of the bridge circuit 11
Is read (step 204). This temperature voltage D _P is
It is the temperature voltage that changes under the influence of the temperature change that changes the zero point of the load cell and the weight W of the article to be weighed placed on the mounting table. Then, the temperature measurement timer is cleared (step 206). Next, in step 200,
If the temperature measurement timer has not timed out and it is determined to be NO, the weight measurement mode is entered, and the CPU 20 turns on the switch SW1 and turns off the switch SW2 (step 208), and the weight W is applied. The load voltage C _P generated at the output terminals 14 and 15 of the bridge circuit 11 is read (step 210), and the read load voltage C _P and D _P read in step 204 are
A new zero point (tare weight voltage) that is substituted in the previously stored equation (8) to compensate for the zero point error caused by temperature changes
C _M is calculated (step 212). The zero point C
_M also compensates for the effect of weight W. Next, this zero point C
By calculating the weight W by substituting _M and the load voltage C _P into the previously stored equation (9), the weight W without error due to temperature can be measured (step 21).
4). Then, the time of the temperature measurement timer is incremented (step 216). However, although the timing of the zero point correction is measured with a timer and is performed at a predetermined time interval, it may be performed irregularly.

A second embodiment will be described with reference to FIG. In the first embodiment, as shown in FIG. 1, the analog weight voltage k ₁
(E ₁ -e ₂ ) and the temperature voltage e ₂ are converted into digital values by one A / D conversion circuit 19, whereas in the second embodiment, as shown in FIG. The switch circuit 18 is omitted, and the weighted voltage k ₁ · (e ₁ −e ₂ ) and the temperature voltage e ₂ are converted into digital values by dedicated A / D conversion circuits 19 and 23, respectively. Other configurations and operations are the same as those of the first embodiment, the same portions are denoted by the same reference numerals, and detailed description thereof will be omitted.

In the first embodiment, the switches SW1 and SW2
By changing the load voltage k ₁ · (e ₁ −e ₂ )
The temperature voltage e ₂ and the temperature voltage e ₂ can be A / D converted by one A / D conversion circuit 19. However, since a predetermined switching time is required to switch the switches SW1 and SW2, the load voltage k that changes at a high speed. It is not suitable for the purpose of faithfully and rapidly A / D converting ₁ · (e ₁ −e ₂ ). On the contrary,
In the second embodiment, the load voltage k ₁ · (e ₁ −e ₂ ) and the temperature voltage e ₂ are separately A / D converted, and the digital values obtained by each A / D conversion are separately stored at any time. Since it can be stored in the unit 22, the temperature-compensated weighted voltage of the zero point can be obtained without delay in timing.

A third embodiment will be described with reference to FIG.
In the first embodiment, as shown in FIG. 1, the power supply voltage E ₁ (=
10 V) is applied to the bridge circuit 11, the temperature sensitive element 12, the amplifiers 16 and 21, and the like, in the third embodiment, as shown in FIG. 14, a power supply voltage + E obtained by providing an analog common. ₂ (= + 5V) and -E ₂ (= -5
V) is a bridge circuit 11, a temperature sensitive element 12, an amplifier 1
It is a structure applied to 6, 21, etc. Other configurations and operations are the same as those of the first embodiment, the same portions are denoted by the same reference numerals, and detailed description thereof will be omitted. However, E ₂ is 5V
However, other voltages may be used.

With the configuration shown in FIG. 14, a temperature voltage e _{2 of} -0.6 V is applied to the output terminal 15, and + E ₂ (= + 5 V) and -E ₂ (= -5 V) are applied to the amplifier 21. The voltage is on. Therefore, the amplification factor k ₂ of the amplifier 21 can be designed to be 5 / 0.6≈8.3.

In the conventional zero correction device shown in FIG. 12, power supply voltages + E ₂ (= + 5V) and -E ₂ (= -5).
Considering a configuration in which V) is applied to the bridge circuit 1, the temperature sensitive resistor 2, the amplifier circuit 4 ′, etc., a voltage of 3.8V is applied to the input terminal 1a, and + E ₂ (= + 5) is applied to the amplifier circuit 4 ′.
V) and -E ₂ (= -5V) voltage is applied. Therefore, the amplification factor k ₂ of the amplifier circuit 4 ′ can be designed to be 5 / 3.8≈1.3. As described above, in the conventional zero-point correction device shown in FIG. 12, the amplification factor k ₂ can be designed only to a small value of about 1.3, while in the third embodiment of the present application, the amplification factor k ₂ is set. Since k ₂ can be designed to be about 8.3, the temperature of the load cell can be measured more accurately than before, and as a result, the zero point correction can be performed with higher accuracy.

The temperature compensating device for the load cell of the first and second embodiments can be applied to, for example, an electronic scale, a combination scale, a weight checker, or the like.

[0050]

According to the first and third aspects of the invention, the temperature voltage (eg, e ₂ ) generated at one output end of the bridge circuit
Since is less than 1/2 of the voltage of the power supply voltage of the bridge circuit (e.g., E _1), the power supply voltage E ₁ of the bridge circuit,
Even when the power supply voltage E ₁ of an amplifier or the like for amplifying the temperature voltage e ₂ is shared, the amplification factor k ₂ of the amplifier is E ₁ / e ₂
> 2, and as a result, the zero point compensation with respect to temperature can be performed accurately, whereas in the conventional example shown in FIG. 12, the power supply voltage V _ey of the amplifier circuit 4 ′ is set to that of the bridge circuit 1. When shared with the power supply voltage V _ex and set to 10 V, for example, the input voltage V input to the amplifier circuit 4 ′ is 8.8 V, so that the amplification factor k _x of the amplifier circuit 4 ′ is 10 / 8.8≈1.
There is a problem in that it is necessary to design it to be less than 1, the amplification factor k _x cannot be designed to be a large value, and as a result, zero compensation with respect to temperature cannot be performed accurately. As a result, in the conventional example, the power supply voltage of the bridge circuit 1 and the amplifier circuit 4 ′ cannot be shared, while the first,
According to the third invention, it is possible to share the power supply voltage of both of them, which has the effect that the circuit becomes simpler and the cost can be kept lower than ever.

Moreover, as in the conventional case, there is an effect that the zero point change due to the temperature change of the load cell can be accurately corrected.

According to the second and fourth inventions, in addition to the effects of the first and third inventions, the temperature sensing element used for temperature measurement electrically changes the output span due to the temperature of the load cell. Since it can be corrected, there is an effect that it is not necessary to provide another temperature-sensitive resistor for temperature compensation of the span.

[Brief description of drawings]

FIG. 1 is a block diagram showing an electric circuit of a weighing device to which a temperature compensating device for a load cell according to a first embodiment of the present invention is applied.

FIG. 2 is a block diagram showing an electric circuit of a weighing device to which a temperature compensating device for a load cell according to a second embodiment of the present invention is applied.

FIG. 3 is a block diagram of a bridge circuit of the first embodiment.

FIG. 4 is a load voltage A and a load cell temperature t of the first embodiment.
It is a figure which shows the relationship with.

FIG. 5 is a temperature voltage B and a load cell temperature t of the first embodiment.
It is a figure which shows the relationship with.

FIG. 6 is a diagram showing a relationship between a load voltage C and a load applied to a load cell according to the first embodiment.

FIG. 7 is a diagram showing a relationship between a temperature voltage D and a load applied to a load cell according to the first embodiment.

FIG. 8 is a diagram showing a relationship between a change amount H of the temperature voltage D and a load cell temperature t in the first embodiment.

FIG. 9 is a flowchart showing a procedure for obtaining a span coefficient in the first embodiment.

FIG. 10 is a flowchart showing a procedure for obtaining a weight independent of temperature by performing zero point correction in the first embodiment.

FIG. 11 is a block diagram in which a conventional zero correction resistor is inserted in a bridge circuit.

FIG. 12 is a block diagram showing an electric circuit of another conventional temperature compensation device.

FIG. 13 is a block diagram showing an electric circuit of still another conventional temperature compensation device.

FIG. 14 is a block diagram showing an electric circuit of a weighing device to which a temperature compensating device for a load cell according to a third embodiment of the present invention is applied.

[Explanation of symbols]

11 bridge circuit 12 Temperature sensor 13 Strain gauge 14, 15 Output end 20 CPU

─────────────────────────────────────────────────── ─── Continuation of the front page (58) Fields surveyed (Int.Cl. ⁷ , DB name) G01L 1/22

Claims (4)

(57) [Claims] 1. A temperature-sensitive element is provided on a strain-generating element of a strain-gauge load cell in which a strain gauge is formed in a bridge circuit, and one end of the temperature-sensitive element is connected to one input end of the bridge circuit. Is connected to the other input end of the bridge circuit, the voltage difference between the output ends of the bridge circuit is amplified by the first amplifier, and the voltage of one output end is increased to the second In a temperature compensating method of a load cell which is amplified by an amplifier and supplies a voltage to the first and second amplifiers from the power source, a zero point change amount C generated at both output ends of the bridge circuit based on a temperature change. the _{M, C M = C 1 -} [(a 2 -A 1) / (B 2 -B 1)] [D
_{-D 1 - (D 2 -D 1} ) (C-C 1) / (C 2 -
C ₁ )] (where C ₁ is the load voltage which is the output voltage of the first amplifier when no article is loaded on the load cell at the reference temperature, and C ₂ is the weight cell of the weight m at the reference temperature. The load voltage when loaded on the load cell, C is the load voltage when a certain load is loaded on the load cell at an arbitrary temperature, and D1 is the second load voltage when no article is loaded on the load cell at the reference temperature. Is the output voltage of the amplifier, D2 is the temperature voltage when a weight of weight m is loaded on the load cell at the reference temperature, and D is a load when the load cell is loaded at the arbitrary temperature. the temperature voltage, a ₁ is the load voltage when the article on the load cell at a first temperature is not loading, a ₂ is in the second temperature The load voltage when the article serial load cell is not loading, B ₁ is the temperature voltage when the article on the load cell at a first temperature is not loading, B ₂ is an article on the load cell at a second temperature Load voltage is calculated based on the temperature voltage when the load voltage is not loaded, and the load voltage generated at both output ends of the bridge circuit is corrected to the zero point based on the zero point change amount. Temperature compensation method. 2. The temperature compensation method for a load cell according to claim 1, wherein the temperature sensing element electrically corrects an output span due to the temperature of the load cell. 3. A bridge circuit including a strain gauge provided on a strain-generating body of a load cell; a temperature-sensitive element provided on the strain-generating body, one end of which is connected to one input end of the bridge circuit; A first power supply connected between the other end of the temperature sensing element and the other input end of the bridge circuit, and a voltage difference between the output end of the bridge circuit and the voltage supplied from the power supply. And a second amplifier that amplifies the voltage at one output end of the bridge circuit and is supplied with voltage from the power supply, and is generated at both output ends of the bridge circuit based on temperature changes. The zero point change amount C _M is _calculated as C _M = C ₁ − [(A ₂ −A ₁ ) / (B ₂ −B ₁ )] [D
_{-D 1 - (D 2 -D 1} ) (C-C 1) / (C 2 -
C ₁ )] (where C ₁ is the load voltage which is the output voltage of the first amplifier when no article is loaded on the load cell at the reference temperature, and C ₂ is the weight cell of the weight m at the reference temperature. The load voltage when loaded on the load cell, C is the load voltage when a certain load is loaded on the load cell at an arbitrary temperature, and D1 is the second load voltage when no article is loaded on the load cell at the reference temperature. Is the output voltage of the amplifier, D2 is the temperature voltage when a weight of weight m is loaded on the load cell at the reference temperature, and D is a load when the load cell is loaded at the arbitrary temperature. The temperature voltage of A
₁ is the load voltage when an article is not loaded on the load cell at a first temperature, A ₂ is the load voltage when an article is not loaded on the load cell at a second temperature, and B ₁ is a first Zero temperature change amount calculating means for calculating the temperature voltage when no article is loaded on the load cell at the temperature of, and B ₂ is the temperature voltage when no article is loaded on the load cell at the second temperature). A temperature compensating device for the load cell, comprising: a compensator for compensating the zero point of the load voltage generated at both output ends of the bridge circuit based on the zero point change amount. 4. The temperature compensating device for a load cell according to claim 3, wherein the temperature sensing element is set to a resistance value that electrically corrects an output span due to the temperature of the load cell.